Introduction to Solid State Physicsproblems after each chapter |
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Page 313
The zone boundaries determined by ( 12 . 1 ) are planes normal to each G at the
midpoint . The first Brillouin zone will be formed from the shortest G ' s , of which
there are twelve given by ( 12 . 7 ) . The zone is therefore the rhombic ...
The zone boundaries determined by ( 12 . 1 ) are planes normal to each G at the
midpoint . The first Brillouin zone will be formed from the shortest G ' s , of which
there are twelve given by ( 12 . 7 ) . The zone is therefore the rhombic ...
Page 314
thus there are two states in the zone per atom , one state for each spin orientation
. This result agrees with our earlier statement that an energy band contains two
states for every atom in the crystal . There are several further points of interest ...
thus there are two states in the zone per atom , one state for each spin orientation
. This result agrees with our earlier statement that an energy band contains two
states for every atom in the crystal . There are several further points of interest ...
Page 326
36 for which the inscribed Fermi sphere makes contact with the Brillouin zone
surface for the foc lattice . The observed electron concentration of the ß phase (
bcc ) is close to the concentration 1 . 48 for which the inscribed Fermi sphere
makes ...
36 for which the inscribed Fermi sphere makes contact with the Brillouin zone
surface for the foc lattice . The observed electron concentration of the ß phase (
bcc ) is close to the concentration 1 . 48 for which the inscribed Fermi sphere
makes ...
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Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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alloys applied approximately associated atoms axis band boundary calculated cell chapter charge concentration condition conductivity consider constant crystal cubic density dependence determined dielectric diffusion direction discussion dislocation distribution domain effect elastic electric electron elements energy equal equation equilibrium experimental expression factor field force frequency function germanium give given heat capacity hexagonal holes important impurity increase interaction ionic ions lattice levels London magnetic mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential present problem properties range reference reflection region relation resistivity result room temperature rotation shown in Fig simple solid solution space space group specimen structure surface symmetry Table temperature theory thermal tion transition unit usually values vector volume wave zero zone